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Turbulent fluctuations at kinetic scales: from coherent structures to quasi-parallel whistler waves

Authors :
Alexandrova, O.
Lacombe, C.
Matteini, Lorenzo
Rossi, C.
Maksimovic, M.
Mangeney, André
Santolík, O.
Cornilleau-Wehrlin, Nicole
De Conchy, Y.
Laboratoire d'études spatiales et d'instrumentation en astrophysique (LESIA)
Université Pierre et Marie Curie - Paris 6 (UPMC)-Institut national des sciences de l'Univers (INSU - CNRS)-Observatoire de Paris
Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Université Paris Diderot - Paris 7 (UPD7)-Centre National de la Recherche Scientifique (CNRS)
Laboratoire de Physique des Plasmas (LPP)
Université Paris-Saclay-Sorbonne Université (SU)-Centre National de la Recherche Scientifique (CNRS)-Université Paris-Sud - Paris 11 (UP11)-École polytechnique (X)-Observatoire de Paris
Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)
Université Paris-Sud - Paris 11 (UP11)-Observatoire de Paris
Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-École polytechnique (X)-Sorbonne Université (SU)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS)
Source :
EGU General Assembly, EGU General Assembly, Apr 2015, Vienna, Austria. 17, 2015
Publication Year :
2015
Publisher :
HAL CCSD, 2015.

Abstract

International audience; The nature of the magnetic field fluctuations in the solar wind between the ion and electron scales is still under debate. Using the Cluster/STAFF instrument, we make a survey of the power spectral density and of the polarization of these fluctuations at frequencies f ∈ [1,400] Hz, during five years (2001-2005) when Cluster was in the free solar wind. In most of the analyzed time intervals, the fluctuations have quasi-random polarization and they have a general spectral shape between the ion scales and a fraction of electron scales. The intensity of these spectra is well correlated to the ion thermal pressure. These fluctuations seem to have a negligible frequency in the solar wind frame, and a wavevector anisotropy k⊥ ≫ k||. Such time intervals are dominated by coherent structures, propagating with a finit velocity in the plasma frame, in the plane perpendicular to the mean magnetic field. In the rest ~ 10% of the selected data, we observe narrow-band, right-handed, circularly polarized fluctuations, with wave vectors quasi-parallel to the mean magnetic field, superimposed on the spectrum of the permanent background turbulence. We interpret these coherent fluctuations as whistler mode waves. The life time of such waves varies between a few seconds and several hours. We analyze in details the long-lived whistler waves, i.e. with a life time longer than five minutes. When the electron parallel beta factor betae|| is larger than 3, the whistler waves are seen along the heat flux threshold of the whistler heat flux instability.

Details

Language :
English
Database :
OpenAIRE
Journal :
EGU General Assembly, EGU General Assembly, Apr 2015, Vienna, Austria. 17, 2015
Accession number :
edsair.dedup.wf.001..28bb477c25724e5b22246bc301bdafa2